Method of and apparatus for the formation of images



N. DEISCH May 7, 1935.

METHOD OF AND APPARATUS FOR THE FORMATION OF IMAGES Filed u1 '22, 1950 5 Sheets-Sheet l II/I/I/IIIIIA IIIIII/IIIIIII/ll/Il/II/III/I/IIIII/Ill!) III/II/IIYIIIIIIII war/1111111 FIG. 3

FIG. 2

May 7,1935, E H 2,000,379

METHOD OF AND APPARATUS FOR THE FORMATION OF IMAGES.

Filed July 22, 1930 s Sheets-Sheet 2 y 7, 1935. N. DEISCH 2,000,379

METHOD OF AND APPARATUS FOR THE FORMATION OF IMAGES Filed July 22, ,1950 5 Sheets-Sheet 3 FIG. 6 0 FIG. 7

zlwuantov- Patented May 7, 1935 g v I UNi'lED STATES PATENT OFFICE METHOD OF AND APPARATUS FOR, THE FGIEEMATION F EMAGES Noel Deisch, Washington, D. (3., assignor of onehalf to Thos. E. Stone, Jr., New York, N. Y.

Application -luly 22, 1930, Serial No. 469,855

19 Claims. (Cl. 178--6) The present invention relates to the formation image-forming system the optical diagram of of images, and its general object is to provide imwhich is shown in Fig. 5, and indicates the method proved means for the translation of the electric by which the inductive strain acting between the current analogue of an image into a real image. electrodes of the one cell is made to be greater Briefly, the apparatus used in the illustrative than that acting within the other cell. 6

embodiment of the invention shown in the draw- Fig. 7 is a diagram corresponding to Fig. 6 but ings comprises a composite electro-optic cell the showing a modification in which the electro-optic electrodes of which consist oi a plurality of linear cells are differently biased. elements, the two sets of electrode elements in- In the transmission of images by the methods 10 tersecting orthogonally to define active areas of phototelegraphy and television, it is usual to 10 located at the points of nearest approach of the scan the image to be transmitted through a electrode elements. A commutator connects succession of coordinate points defining a mosaic, the electrode elements in cyclic progression to the scanning process consisting essentially in the line carrying the modulated current which exdetermining the density of the image at a; s uccesl5 cites the electrodes. Polarized light enters sion of points and restating these density deterl5 obliquely the interspaces between the upper elecminations in terms of some characteristic of an trode elements, and is reflected back through electric current. The two dimensional optical these interspaces by the lower electrode elements. image is thus translated into a single dimensional In its passage the light is modified at a plurality of electrical analogue, the variations of the paramintersection points by the strained dielectric, the eters of which analogue in time are coordinate 2O magnitude of the modification depending on the with the variations of density of the scanned order or" the strain at these points, and this modiimage in space. This electric current analogue fication is detected by means of an analyzer. The may be further converted into an electromagnetic dielectric is chosen as one subject to inertia, so disturbance of the I-Iertzian type. At the station that the period of optical strain is prolonged where the image is to be reconstituted, charac- 2.; beyond the period of electrical stress. The efiect teristics of successive points along the analogue of unequal spectral retardation is overcome by are. translated into approximations of the density using lights of complementary hues, subjecting of corresponding coordinate points of the original these hues separately to stresses producing equal image. It is with this process of re-translating relative retardationsin the two beams, and comthe electric current analogue of an image into a L 0 bining the hues to produce white. real image that the present invention more par- Referring to the drawings: ticularly deals. Fig. l is a diagram showing the optical arrange'' In Fig. 1 there is shown a projection system ment of an image-forming system made accordcomprising a Source Of radiation l, a polarizer 2, ing to the present invention. an absorbing screen 3 adapted to select a prefer- Fig. 2 is an enlarged iragmental section of the ably restricted region from the spectrum of. the electro-optic cell taken on the line 2-2 of Fig. 1, radiation emitted by the source I, a collimating and shows especially the arrangement of the lens 4, an electro-optic cell assembly 5, an imaglatticed electrodes, their retaining plates, the ing lens G, an analyzer 'l, and a diffusing screen l0 dielectric, and the path of the incident and. 8. The polarizer 2 and the analyzer 1 may con- 40 emergent light beams. sist of Nicolprisms, the construction of which is Fig. 3 is an enlarged iragmental section taken well known. The Nicol 2 is preferably turned on on the line 33 of Fig. 2. its longitudinal axis through an azimuth of Fig. 4 is an electrical circuit diagram showing with respect to a plane passing through theaxis 45' the arrangement of the latticed electrodes in the of strain existing between the electrodes of the electro-optic cell, the commutator mechanism, electro-optic cell 5, whereas the principal plane and the line connection to an illustrative radio of the analyzer l is desirably but not necessarily receiving circuit. held orthogonal with this axis of strain.

Fig. 5 is a diagram showing the optical ar- The electro-optic cell 5 comprises electrodes I0 rangement of a projection system in which two (Figs. 2 and 3) and H, each including elements separate but coordinate image-forming systems lBa, lllb, lflc, etc., and Ila, H2), H0, etc., retransmitting respectively lights of complementary spectively. The elements 10a, 10b, 100, etc., of hues, are used to nullify the effect of unequal rethe electrode it! are linear in character, and in tardation in the electro-optic cells. the illustrative case shown are, for a purpose Fig. 6 is an electrical circuit diagram of an which will presently become apparent, provided with inclined faces l3.

These elements are imbedded in V-shaped troughs I2 in the transparent and insulating supporting plate I3. The electrode it with its support It may be formed by ruling troughs in a glass plate, coating (as by mechanical, chemical, or electrical deposition) a conducting substance such as silver over the surface of the plate, and then removing exposed portions of the metallic coating with a fiat tool until the plane of the plate is reached, leaving the electrode portions lea, ifib, lilo, etc, in the grooves I2.

The electrodes Ila, Ilb, llc, etc., are also linear in character, with preferably plane and specular top surfaces i l, and are held on an insulating and preferably opaque support It consisting of a material such as black or deeply stained glass. Ihe electrode assembly ll with its support may be made by coating a plane slab of a suitable material such as black glass with a thin layer of metal, polishing the metal to a specular surface, and then ruling grooves It in the plate, whereby the electrode elements Ila, llb, llc, etc., are left. With this method of constructing the electrodes Ill and l l, by which each electrode element is supported throughout its length, it is possible to produce a very compact electrode assembly, the electrode elements of which are held accurately in the'desired spatial relation.

The electrode elements Illa, Illb, Illc, etc., and I la,.! lb, I I0, etc., in each of the electrodes are in the illustrative case parallel and coplanar, and the elements in the two sets of electrodes are held mutually perpendicular to each other, as shown in Figs. 2, 3, and 4, in such manner that the electrodes form an intersecting lattice. A plurality of independent electro-optic cells arranged as a mosaic are thus formed at the intersections of the electrode elements. The spacing intervals 8, Fig. 3, of the electrode elements lea, Illb, lilo, etc., is in the illustrative arrangement of the cell preferabfy made greater than the spacing interval s, Fig. 2; of the electrode elements Ila, llb, Ilc, etc., to compensate the optical foreshortening consequent on anoblique incidence of light.

The space between the electrodes l0 and II is filled with an electro-optically active substance Il, which when subjected to electric strain, as by a dilference of potential existing between members of the elements Illa, lbb, lllc, etc., and Ila, Ilb, ll 0, etc., becomes birefringent, according to the well-known Kerr and analogous effects. dielectric may consist of nitrobenzol, as ordinarily used in electro-optic cells, but, for a purpose that will later be explained, it preferably consists of a substance having a high electro-optic' lag, such as one of the higher alcohols, e. g., undecyl alcohol, or a viscous vegetable oil, such as castor oil.

The assembly above described constitutes in effect a composite electro-optic cell, the unit cells, which are arranged as a mosaic, being defined by crossing electrodes, and including the intervening dielectric space. It will be observed that these unit cells are arranged in parallel rows, and that each unit cell is a member of two rows lying along perpendicular directional axes. All of the cells in each row along a certain directional axis have an electrode of one polarity in common, and all of the cells in each row along an axis perpendicular to the first axis have an electrode of opposite polarity in common. The cells have also a common dielectric.

The electrode supports I3 and I5 are held in a frame 20, Fig. l, which latter maintains the This proper separation between the electrodes and serves to prevent escape of the dielectric H. To prevent surface reflection of light at the otherwise glass-air interface of the electrode support I3, a rhomboidal prism 2!, Fig. 1, having plane enterthe upper plane face of the prism 2i, as shown in Fig. 1.

Light from the'source I is polarized by the prism 2, and after passage through the filter 3, is collimated into a parallel bundle by the lens 4. It

then passes into the prism 2i and the electrode support 53. Referring now .to Fig. 3 it will be seen that the incident beam of light, a portion of which is shown as of the width T, falls into the plane of the electrode It, where portions of the beam strike the inclined faces lb of the electrode elements lea, Illb, Illc,etc., and'are reflected vertically in narrow parallel bundles 23, which fall upon the roof plate 22 of the cell 5 and are ab sorbed. Other portions 2d of the beam pass through the interspaces I9 between the electrode elements Illa, Iflb, IGc, etc., and fall into the plane of the lower electrode II. light fall upon the reflecting surfaces M of the electrode elements l Ia, I Ib, l Ic, etc, and arerefiected back through the interspaces I9 between the electrode elements Illa, Mb, I00, etc. The intervening portions of the beams 2 3 fall upon the inclined faces of the grooves It, by which they become trapped and are caused to be absorbed by the opaque support I5.

The collimated beam entering the cell 5 is hence first divided into a number of thin parallel ribbons of light 24, and these are further divided into a number of separate narrow square pencils of light 24, Figs. 2 and 8 It Will be noted that each of the pencils of light as passes between a separate intersection of the electrode elements ltd, lllb, Iflc, etc., and Ila, Ilb, llc,,etc. These Here portions of the pencils emerge from the face 26 of the prism 2i, V

are converged by the lens ii, and pass through the analyzer l, whence they diverge and fall upon the screen 8, forming a mosaic pattern of square dots analogous to the dots of a half-tone screen.

and lie, Fig. 2, the space shown at 2! inFigs. 2 r

and 3 comprised between the nearest point of approach of these electrodes becomes subject to 7 electric strain, and the dielectric I? at this area becomes birefringent. As above mentioned the polarizing nicol 2 is preferably oriented atan azimuth of 45 with respect to the plane passing through the axis of electric strain. Thus the plane of polarization of the plane polarized light entering the space between the elements lt b and I I0 lies at an azimuth of 45 with respect to the principal axis of the Faraday tubes of force "constitutingthe field between the electrode e1ements.-

Due to the birefringence set up in the dielectric, the plane polarized light entering the strained space becomes elliptically-polarized, the axes of ellipticity being respectively parallel with and perpendicular to the axis of the tubes of force of the electric field. The pencil of polarized light 241 which traverses this strained space'is hence subtil ject to a certain retardation, the order of which with a given dielectric and with a cell of given dimensions is determined by the magnitude of the diiference of potential between the two electrodes causing the strain. The principal plane of the analyzing Nicol is, as abovestated, preferably held orthogonal to the axis of strain existing between the electrodes of the electro-optic cell 5.

It thus lies in one of the axes of ellipticity' of the elliptically polarized light constituting the pencils 24. Under these conditions the quantity of light passing the Nicol l is determined by the degree of ellipticity of this light. Since the ellipticity of these pencils changes with the retardation, the transmission of the pencils 24 by the Nicol 7 also changes with the retardation. The particular pencil of polarized light above referred to is hence transmitted in the analyzer in amount dependent on the excitation of the electrodes It and Ii, and the dot projected on the screen 8 is of a corresponding brightness. The mean or continuous transmission for all of the pencils 24, that is, the transmissionwhen the incoming signal is unmodulated, depends, other conditions being equal, on the permanent ornormal electrical bias existing between the electrodes it and H of the cell 5, since this bias determines the permanent state of ellipticity in the emergent beams 24. The value of this bias in the circuit shown in Fig. 4 and hereafter to be described, is determined by the relation between thenormal static space current passed by the tube 31, and the ohmic value of the resistance 40. Nicols 2 and oriented as described above, this bias is preferably but not necessarily chosen to be such that the ratio of the axes of the elliptically polarized light constituting the pencils 24' is infinite, giving plane polarized light. The plane of polarization will be perpendicular to the principal plane of the Nicol With this condition obtaining, and with no modulation active, the Nicol l extinguishes the light constituting each of the pencils 24 and the screen 8 is dark. Modulations through a certain value above the level of this bias cause the ellipticity to change through successive values and finally to become infinite in a plane perpendicular to the former plane, again corresponding to plane polarized light, but with the plane of polarization perpendicular to that which first obtained. The light constituting the pencil aifected is in this case completely transmitted, since this second plane corresponds with the principal plane of the prism a. In the normal operation of the apparatus the depth of modulation measuring the extreme highlights and the extreme shadows of the transmitted picture correspond to these two limits.

Although only one pair of intersections of the elements of the electrodes l8 and I I may be activated by the modulating current at one time, still,

for reasons presently to be developed, several or' many of the. pencils projected on the screen may be affected as to brightness simultaneously. Further, though the individual spots of light which fall on the screen may be rapidly changing in brightness due to modulations, they are fused by the persistence of vision into a homogeneous eifect. It is hence apparent that with each of the pencils of light 24 receiving the proper retardation-a mosaic picture is produced on the screen 8.

In Fig. 4 is shown the apparatus by which the electrodes H and H are ener ized in the process of converting the electrical analogue of the transmitted image into a real image. The incoming With the assumed to be a modulated carrier wave, is received on the aerial 35. The received signal is selected and amplified in the apparatus 36, which is shown as a radio receiving set of conventional design. The rectified current from the detecting tube 3! creates a difiference of potential across the leads 38 and 39, the'magnitude of which potential varies according to the modulations of the received signal. A resistance 40 is placed between the leads 38 and 39 to allow of the readjustment of the potential across these leads between 5110- cessive modulations.

The leads 38 and 39 have connection respectively with the brushes 4| and 42 of the commutators 43 and 44. All but one of the sectors 45 of the commutator 43 has connection through a lead 41 with one of the electrode elements Illa, I012, I00, etc., and each of the sectors 46 of the commutator 44 has connection through the leads 48 with one of the electrode elements Ila, llb, ||c, etc. Means are thus provided for individually and selectively exciting any given pair of opposed electrode elements. shown 23 of the elements IOa, lob, |c, etc., and 24 of the elements I Ia, |b,'| |c, etc. These numbers are merely illustrative however, and in a givenapparatus it might be desirable to include a much greater number of elements than that shown.

The brush 4| has mechanical connection through the shaft 50 with the motor M, by which it is turned to make connection with the sectors 45 of the commutator 43.- An insulating coupling in the shaft 50 serves to localize the electric charge on the brush 4|. On a prolongation 52 of themotor shaft 50 is carried the pinion 53, which drives, through the train of reducing gearing 54 and the shaft 55, in which is intercalated the insulating coupling 56, the brush 42. The reduction,

gearing 54 is shown as having the reduction ratio 24 11; thus the brush 4| of the commutator 43 makes contact with each of the 24 segments of the commutator 43 while the brush 42 is contacting one sector 46 of the commutator 44. It

wlll'be noted that a blind sector 45' is provided in the commutator 43 which is passed over by the In the drawing there are brush 4| during the time the brush 42 is passing through direct metallic contact. However, other forms of commutator are known, such as those which operate through electromagnetic or electrostatic induction, through conductivity induced by light action, or by the deflection of a cathode beam, and it will be understood that I do not wish to limit myself tothe use of the illustrative commutator.

Since each one of the electrode elements of the electrode N, Fig. 4, remains connected with line 39'during the time that all of the several elements of the electrode ID are connected in succession with line 38', all of the unit areas located between intersections of the elements of the electrodes l0 and II are momentarily excited, ac-

cording to a periodic succession, the degree of the excitation corresponding to the depth of the modulation of the electric current analogue.

Each unit cell of the composite electro-optic cell is thus excited only a fraction of the total time taken to complete a cycle of contacts, and it, is hence of advantage that the effects of this excitation be prolonged beyond the period of actual alcohol castor oil as being suitable for the purpose, though of course I do not wish. to limit myself to the use of these particular materials.

It is well known that in seeking to secure the reproduction of an image by the use of methods which involve the introduction of retardation in a beam of polarized light, as by means of a Kerr cell in which a dielectric is electrically strained h to producebireiringence, lights of different wavelengths are subject to difierent degrees of relativeretardation, resulting in a change in spectral composition of the light when the latter is passed through an analyzer. For this reason a polarized beam of white light after passage through such a cell and through its accompanying analyzer is usually brilliantly colored, the exact hue depending on the order of the retardation in the cell. If it be attempted to use white light in securing a directly visual, image, using such a cell as an intermediary, the image will be highly colored in a most erratic way. This effect makes it impracticable touse such a cell by ordinary methods for securing a directly visual image. The above effect can be mitigated to some extent by using light of practically one degree of re frangibility. for transmission through the cell. .In this case the image is uniformly but brilliantly colored, which fact makes the field of; application of this method very limited. v,

To overcome this diff culty I use atleast two kinds of light each ofdifierent huein forming a single image. The hues are chosen as complementaries, such as yellow-green and violet, or

yellow and indigo, or orangeand blue, or red and blue,green, any of which-pairs of hues will produce white additively when combined in proper proportion. These polarized lights are separately subjectedto proportional retardations to produce equal extinctions when passed through analyzers,

and the lights and then combined to produce white.v v V Fig. 5 makes clear the opticalarrangement by which this method of working is carried into.

practice. The apparatus includes two separate but associated optical systems 58 and59, having similar parts, consisting of sources Gil, polarizers 6|, filters 62 and 63, collimators 54, electro-optic cell assemblies 65 and 66. which may be of the type shown at 5 in Fig. l, analyzers Bl, diverging lenses 68, deflecting prisms 6s and lo, and a diffusing screen H. The color screen 62 is made to pass a preferably narrow band of radiation of one complementary hue, say red, and; the other is such as will pass 2. preferably narrow band of radiation of a second complementary hue, bluegreen. The prisms 69 and Ill arearranged to bend their respective beams obliquely toward the centre of the screen to securesubstantial coincidence oi the mosaic patterns formed in the two Many methods of unitmodulating current, as by means such as shown in Fig. i, is that of using a dielectric of such Kerr constant in each cell that the proper retardations.

are obtained for each color used. Dielectrics of a wide range of sensibility can be readily prepared by mixing in various proportions two mutually miscible dielectric liquids of different Kerr constants, such as nitrobenzol with a Kerr constant of 256x10 and benzol with a Kerr constant O.6 lil- Assume that the cell 65 transmits orange and is filled with a dielectric consisting of nitrobenzol. The celllifi transmits blue, which requires smaller birefringence to induce a given proportional retardation; it will hence be filled with a' certain dilution of nitrobenzol. The proper dilution for a given assembly may be determined by computation, or empirically by using successively greater dilutions until the proper mixture is had. i

Two electrical methods are shown in Figs. 6 and 7 respectively, by which the cells and 66 can be made to produce proportional retardation's; even when both of these cells contain a 1;

dielectric of thesame composition. Referring to Fig. 6, it will be seen that the elements 853. of the electro-o-ptic cell as have connection, with the segments of the commutator 85, and the ele ments 8! of-the cell 55 have connection with the segments of the commutator 84, substantially as 7 described in connection with Fig. l. Likewise the elements 83 of the electro-optic cell '66 have,

connection with the segments of the commutator 86 and the elements 82 have-connection-wlth the segments of the commutator 81. The brushes 88 and 39 have commonconnectionto onepole of the battery 92. through the'lead 99 and the portion 5-33 of the secondary 96 of the mututal inductance coil 9% with theopposite pole of the battery 92, whereas the brush Eli has connection through the entire length of the secondary M, of the inductance coil 96 with the battery 92. Thebrushes 88 and S9,

and the brushes es and 3!, are rotated uniformly and ccnjointly, by means such as those shown in Fig. l. The terminals 9'! and 98 of the pris mary 95 of the mutual inductance as receive the modulated current representing the analogue of the image to be reproduced; these leads may correspond to the leads-38 and th of Fig. 4. The function of the battery 92 is to bias the electrodes of the electro-optic cells and 6B, thus giving them added sensibility to impulses that may-be superposed on this bias.

An impulse in the leads 9? and 98 setsup a fieldinthe primary winding of the .mutual inductance coil 95 a portion-of the energy of which is transferred to the secondary winding 9%, in which it sets up a difference of potential. Due to the point of insertion of the lead 89 into the convolutions of the coil M, only a portion of the total difference of potential set up in'this coil is impressed across the electrodes tiland 8|. This electrical stress results in a corresponding die- The brush 96 has connection.

gree'of birefringence being set up in the electrooptic cell 65, which transmits light of a certain color, say blue-green. However the full difference of potential induced in the secondary 94 is impressed on the electrodes of the electro-optic cell 66, to set up a birefringence of corresponding value in the dielectric of this cell, which transmits a certain other color, say red. By choosing proper values for the inductances 93 and 94, the degrees of birefringence set up in the two cells may be made to suit the particular set of light complementaries employed.

In the modification shown in Fig. 7, the brush,

88' of the cell 65', and the brush 89' of the cell 66 are connected to the lead I09. The brush 9!) of the cell 65' has connection through the battery I02 to the lead NH, and the brush 9| of the cell 66' has connection through the batteries I03 and I02 to the lead "H. The terminals Hill and HH may correspond to the leads'38 and 39, Fig. 4. Impulses across these leads become incident on the electrodes of the cells 65' and 66' through their respective brushes and commutators. The cell 65 receives a certain bias from the battery I82, whereas the cell 66 receives a bias due to the combined action of the batteries I82 and I03. The cell 66' has thereforea greater inherent sensibility to electric'impulses than the cell 65'. By properly choosing the values of the biases impressed on the cells 55' and 65', the degrees of birefringence set up in the two cells maybe made to suit the particular set of light complementaries employed.

It is well known that the visual effect corresponding to white may be produced by the admixture of three or more hues, and though I have for convenience shown the use of but two hues in the above description, I do not desire to be limited to this number.

While I have described my invention with re spect to the preferred form' thereof, I reserve the right to make such changes in the details of construction or such substitution of equivalents as conform to the spirit of the invention or fall within its scope as defined by the appended claims. It is moreover not indispensable that all features .of the invention be used conjointly, as they may be advantageously employed in various combinations or subcombinations.

I claim: v

1. In an apparatus for the formation of images from an electric current analogue, an electro-opticcell comprising a composite electrode including a plurality of electrode-elements separated by interspaces, a second and reflecting electrode having its reflecting face directed toward said composite electrode, a birefringent member placed between said composite electrodes and said reflecting electrode, and means to pass polarized light through the interspaces in said composite electrode, through said birefringent member, and on to said reflecting electrode, whereby the plane of polarization of said light is rotated, and said light is reflected back through the interspaces of said composite electrode.

2. An apparatus for the formation of images from an electric current analogue comprising a Kerr cell having a plurality of parallel linear electrodes defining one coordinate of a plane image, a plurality of parallel linear electrodes one side of which constitutes a reflecting member, said electrodes being arranged at an angle with said first linearelectrodes defining a second coordinate of a plane image, the axes of said two sets of electrodes lying in different but substantially parallel planes, a birefringent member between said electrodes, and'means for progressively subjecting members of said electrodes to a difference of potential corresponding to modulations inv said electric current analogue whereby the medium between said electrodes is subjected to an electric stress andbecomes birefringent. 1

3. In apparatus for converting an electric analogue of an image into a real image, a composite electro-optic cell involving a plurality of unit electro-optic cells arranged in rows paralleling differentdirectional axes, each of said cells including opposite spaced electrodes having a birefringent member therebetween each cell a member of at least two rows lying on different directional axes, independently energizable conductor's connecting an electrode of all cells in each row parallel to one directional axis, independently energizable conductors connecting a different electrode of all cells in each row parallel to another directional axis, the connections made by said conductors being respectively in the directions of the two respective axes, means to pass polarized light through said cells, and means to convert changes of polarization of said light of brightness.

4. In apparatus for converting an electric analogue of an image into a real image, a composite Kerr cell involving a plurality of unit Kerr cells having a common dielectric, said cells ar# ranged in rows having different axes of symmetry, all the cells in each row along one axis of symmetry having an electrode of one polarity in common, all the cells ineach row along another axis of-symmetry having an electrode of another polarity in common, means to pass polarized light through said cell, and means to convert changes of polarization of said light effected by said cell into corresponding changes of bright ness.

5. In apparatus for converting an electric analogue of an image into a real image, an electrooptic'cell comprising a composite electrode including a plurality of spaced elements, a second and reflectingelectrode adapted to co-act with said first electrode and to reflect light back through the interspaces of said first electrode, a birefringent member between said electrodes for rotating the plane of polarized light, and means for passing a beam of polarized light through the interspaces of said first electrode to form nonparallel incident and reflected beams the included angle of said beams being subtended by the centres of adjacent interspaces, whereby the refiected beams are not occulted by the elements of said first electrode.

6. In apparatus. for converting an electric analogue of an image into a-real image, an electro-optic ceIlcomprising acomposite electrode including a plurality of spaced elements, asec-' ond and reflecting electrode adapted to co-act with said first electrodeand to reflect light back through the interspaces of said firstw electrode, a birefringent member between said electrodes for rotatingthe plane of polarized light, and means to pass a beam of polarized light through the in-' terspaces of said first electrode at an angle to the plane of'said first electrode, said angle being substantiallyequal to the complement of half the included angle defined by said interspaces of said first electrode as measured from a point located on said reflecting. electrode midway between said interspaces, whereby light entering through each interspace is reflected back through an adjacent lnterspace.

7. In apparatus for translating the electric current analogue of an image into a real image, said apparatus including electro-optic cells adapted to change theretardation of light transmitted by said cells, the method of balancing the effects of unequal spectral retardation produced in such cells which consists in using more than one light component, said components beingrespectively of such spectral character that onfusion they produce white, passing each of said components through separate cells which produce equal relative retardation, and uniting said components.

8.'An apparatus for the formation of images comprising a Kerr cell having a plurality of separated electrodes including members arranged transversely of and in. proximity to other members thereof to define restricted areas of opposition,'the axes of said transversely arranged members lying in different parallel planes, a birefringent dielectric in the interstitial space between said opposed electrodes, means for passing a beam of polarized light through said birefringent dielectric, and means for impressing different potentials across selected electrodes in sequence and in timed relationship.

9. An apparatus for the formation of images comprising a Kerr cell having a plurality of electrodes including cathode and anode elements, said cathode elements lying transversely of and being separated from said anode elements, the

axes of said cathode elements lying in a plane separated from but parallel with the plane containing the axes of said anode elements, a birefringent dielectric in the space intervening between said cathode and anode elements, the electrode elements on one side of said birefringent dielectric having specular surfaces facing the electrodes on the other side of said birefringent dielectric meansfor passing a beam of light between some of said electrodes and through said birefringent dielectric, a polarizer disposed in said beam before it enters said cell, means for impressing different potentials across selected anode and cathode elements in sequence and in timed relationship, and means including an analyzer disposed in said beam after it emerges from said cell to convert the modifications of polarization sustained by said light in its passage through said dielectric into a visible effect.

10. In apparatus for the formation of images, a Kerr cell comprising a composite electrode including a plurality of spaced elements, means to pass light obliquely between the elements of said electrode, said elements having specular faces to reflect away portions of the incident light which do not pass between said elements, a second composite electrode including a plurality of spaced elements having specular faces to return light which has passed between the elements of said first electrode back through the elements of said first electrode, and a birefringent member between the electrodes.

11. In television receiving apparatus, means to convert an electromagnetic wave analogue of an image into the electric current analogue of said image, image forming means including a K'err cell comprising a plurality of electrodes including cathode and anode elements, the axes of said cathode elements lying in a different parallel plane from and crossing said anode elemerits, a birefringent dielectric separating said anode elements from said cathode elements, the electrodes on one side of said birefringent dielectric having reflecting faces in opposition .to the electrodes on the other side of said birefringent dielectric and means including a commutator to impress different portions in point of time of said electric current analogue on to different electrodes of said Kerr cell.

12. Television apparatus including a radio receiving circuit for converting an ether wave analogue of an image into the electric current analogue of said image, output leads from said receiving circuit, a composite electroeoptic cell involving a plurality of unit Kerr cells arranged in rows paralleling different directional axes, each of said cells comprising two electrodes separated by a birefringent member, each cella member of at least two rows lying on different directional axes, conductors connecting all cells in each row parallel to one directional axis, said conductors being electrically insulated the one from the other, means for selectively placing said conductors in electrical connection with one of said out-; put leads, conductors connecting all cells inea'ch row parallel to another directional said conductors being electrically insulated the one from the other, and means for selectively placing said conductors in electrical connection with an other of said output leads.

13. An apparatus for the formation of images from an electric current analogue including a Kerr cell having electrode elements arranged in sets, said electrodes being disposed-so that the elements of distinct sets intersect each other, and a birefringent member in the interstitialspace defined by said intersections of said electrodes said birefringent member consisting of a higher alcohol such as undecyl alcohol. 14. An apparatus for the formation of images from an electric current analogue including ,a Kerr cell having electrode elements arranged in sets, said electrodes being disposed so that the elements of distinct sets intersect each other, and a birefringent member in the interstitial space defined by said intersections of said electrodes, said birefringent members consisting of castor oil.

15. An apparatus for converting the electric current analogue of an image having portions corresponding to greater and lesser light intensity into a substantially colorless real image, said apparatus including means .to produce separate beams of light of complementary colors, means to polarize each of said beams of light, a Kerr cell for each of said beams to simultaneously change the plane of. polarization of said beams of polarized light through different angles of azimuth re-' sponsive to portions of said analogue corresponding to different light intensities, the absolute rotatory power of said cellsas measured by monochromatic radiation being lesser in the cell transmitting the color of shorter wave-length, and greater in the cell transmitting the complemen tary color of greater wave-length, whereby the angles of rotation in the separate complementary beams are equal for portions of said analogue corresponding to a given image density and the intensity ratio of the two beams remains constant for all degrees of light transmission, analyzers to convey said azimuth changes into corresponding intensity changes in said beam, and means to unite said beams to produce a single visual effect. 16. An apparatus for converting the electric current analogue of an image having portions corresponding to greater and less light intensity into a substantially colorless real image, said ap-' paratus including means to produce separate beams of light of complementary colors, means to polarize each of said beams of light, a Kerr cell for each of said beams to simultaneously change the plane of polarization of said beams of polarized light through different angles of azimuth responsive to portions of said analogue corresponding to different light intensities, the birefringent member within the cell transmitting the beam of shorter wave length having a lower Kerr constant than the birefringent member Within the cell transmitting the beam of longer Wave length, whereby the angles of rotation in the separate complementary beams are equal for portions of said analogue correspondingto a given image density and the intensity ratio of the two beams remains constant for all degrees of light transmission, analyzers to convey said azimuth changes into corresponding intensity changes in said beams, and means to unite said beams to produce a single visual effect.

17. An apparatus for converting the electric current analogue of an image having portions corresponding to greater and lesser light intensity into a substantially colorless real image, said apparatus including means to produce separate beams of light of complementary colors, means to polarize each of said beams of light, a Kerr cell for each of said beams to simultaneously change the plane of polarization of said beams of polarized light through different angles of azimuth responsive to portions of said analogue corresponding to diiferent light intensities, means to produce differences of potential between the electrodes of said cells, said means being responsive to changes in said analogue, the cell transmitting the beam of shorter wave length having a smaller difierence of potential impressed upon its electrodes than the cell transmitting the beam of higher Wave length, whereby the angles of rotation in the separate complementary beams are equal for portions of said analogue corresponding to a given image density and the intensity ratio of the two beams remains constant for all degrees of light transmission, analyzers to convert said azimuth changes into corresponding intensity changes in said beams, and means to unite said beams to produce a single visual efiect.

18. An apparatus for converting the electric current analogue of an image having portions corresponding to greater and lesser light intensity into a substantially colorless real image, said apparatus including means to produce separate beams of light of complementary colors, means to polarize each of said beams of light, a Kerr cell for each of said beams to simultaneously change the plane of polarization of said beams of polarized light through different angles of azimuth responsive to portions of said analogue corresponding to different light intensities, a source of electromotive force to maintain a higher difference of potential across the electrodes of the cell transmitting the beam of longer Wave length than concurrently exists across the electrodes of the cell transmitting the beam of shorter Wave length, whereby the angles of rotation in the separate complementary beams are equal for portions of said analogue corresponding to a given image density and the intensity ratio of the two beams remains constant for all degrees of light transmission, analyzers to convert said azimuth changes into corresponding intensity changes in said beams, and means to unite said beams t produce a single visual effect.

19. The method of translating the electric current analogue of an image into a substantially colorless real image which consists inproducing two beams of polarized light of complementary color, subjecting said beams of light separately to a retarding action in a Kerr cell, applying a potential to the cell that passes the beam of longer wave length in order to subject both beams to equal relative retardation and uniting said beams.

NOEL DEISCH. 

